Part Two of the Second Session of Course 18

When there is no relatively local Kaeler-Metric present for a given arbitrary set of adjacent superstrings, at a general locus in the substringular:  After BRST, the superstrings of discrete energy permittivity and their counterparts AS WELL as their correlative Fadeev-Popov-Trace eigenstates, which are of discrete energy impedance -- and their directly corresponding light-cone-gauge eigenstates, go into the correlative Regge Action eigenmetric, via the correlative Regge Slope, while then going into the generally unnoticed duration of Ultimon Flow.  When there is a relatively local Kaeler-Metric present for a given arbitrary set of adjacent superstrings, at a general locus in the substringular:  After BRST, the superstrings of discrete energy permittivity and their counterparts AS WELL as their correlative Fadeev-Popov-Trace eigenstates, which are of discrete energy impedance -- and their directly corresponding light-cone-gauge eigenstates, go into the directly correlative Klein Bottle eigenstate -- in so as to work to complete one iterative stage of the said Kaeler-Metric, at which point in gauge-metric, the so-stated substringular phenomena that enters the so-eluded-to Schotky Construction re-contracts back to the scalar magnitude of that condition that would be indicative of a completely Lorentz-Contracted condition.  After this entering into the said Klein Bottle eigenstate, the so-eluded-to substringular phenomena shakes eight times back-and-forth in so as to work to cause the shook phenomena to re-attain the needed fractals of respective discrete energy permittvity and its counterpart and discrete energy impedance and its counterpart -- while then going into the correlative Regge Action eigenmetric via the correlative Regge Slope, while then going into the generally unnoticed duration of Ultimon Flow.  This is enough to absorb for now!  Sincerely, Sam.

The First Set of Test Questions For The Last Test Of Course 16

1)  What is a Doubolt cohomology?

2)  What is a Rham cohomology?

3)  Explain how ghost anomalies are annhilated.

4) What are the Donaldson-Ulenbach-Yau conditions?

5)  What is the Bette Action?

6)  What is the Polyakov Action?

7)  What is the Regge Slope?

8)  What makes superstrings oriented?

9)  What makes superstrings unoriented?

10) What is a Klein Bottle eigenstate?

11)  Describe the mobiaty of superstrings.

12)  Describe the mobiaty of world-sheets.

13)  What are Ward conditions?

Part Two of the Just Started Session of Course 16

At this point, consider the directly associated Regge Slope eigenstate that corresponds to the given arbitrary superstring and its correlative counterpart, as the kinematic activity of the so-stated Regge Slope eigenstate happens during the gauge-metric of the integrand locant-based metric -- that would here be directly associated with the iteration of group instanton that corresponds to the portion of the duration of the said multiplicit instanton, that happens right after the corresponding metric or sub-metric of BRST -- during which the so-eluded to superstring is then here redelineated in such a manner in so as to be able to potentially "grasp" another chance to be able to be orientable.  This is if the case in the given arbitrary scenario, if it is that the given so-stated superstring was unorientable over the directly prior eigenmetric of that Bette Action index, that happened over the eluded to iteration of the simultaneous eigenstate of Polyakov Action -- the two different geni of kinematic activity mentioned here, of which happens at the same general duration when taken through the vantage point of a central conipoint in space.  Now, try to think about the Gaussian conditions of the differentiable subspaces of the said string, as it works to correspond to its directly associated superstring and its counterpart -- over the course of the iteration of the eluded-to eigenmetric of Regge Action.  The trajectoral path of the Regge Action is the Regge Slope.  If the supplemental delineation of those waves of core-field-density that are outwardly extended by the said prior kinematic activity of the directly corresponding Bette Action eigenstate -- as these densely distributed segments of mini-string, that bear a certain degree of torsionability, via the activity of the said eigenstate of the Polyakov Action -- will bear indices that work to orientate the directly affiliated Rarita Structure eigenstates that are most local to the activity that I am describing, on account of the "effort" of the said superstring, to bear a certain degree of renormalization with its counterpart.  If the resulting Gaussian of the just eluded-to inter-relationship works to bear an even function of wave-output --that extends from the general center-state, that may be subtended from in-between the so-stated superstring and its counterpart, over the so-stated Regge Action, then, there will be a genus of homeomorphicity that will then form between the said superstring and its counterpart, as this eluded-to phenomenology is pulled through the said Regge Slope eigenstate, which will make the superstring orientable.  If there is, instead, an odd function of wave output that extends from the so-stated center of substringular interaction, then, the superstring will remain as unorientable, and thus, the superstring will here become tachyonic.

A Little Bit About Changes In Symmetry

A superstring that is orientable differentiates kinematically via Noether Flow. A superstring that is not orientable differentiates kinematically via a tachyonic flow. A superstring is orientable when the substringular field eigenstates that are first-ordered and supplementally norm between a given superstring and its corresponding counterstring are trivially isomorpphic in terms of the connections in-between the associated superstring and its corresponding counterstring as caused by the Bette Action, and if the delineatory amplitudes of these said connections have the same scalar distribution when considering all of the said first-ordered substringular field eigenstates, even if the Hodge distribution among the said field eigenstates is not homogeneous and therefore not integrably hermitian during the Laplacian condition of the given instanton in which the associated Bette Action is occurring through its described gauge-metric. If a superstring is not orientable during the Bette Action, the superstring described will attempt to become orientable during the subsequent gauge-metric of a given Regge Action via a Regge Slope that "totters" the associated superstring in an attempt to obtain the multiplicit trivial isomorphism and a common homogeneous and delineatory amplitude that bears a supplementally norm abelian nature that retains the Noether Condition of the said superstring's wave-tug. (This is via a simultaneous internal push-and pull that is exterially projected along the ultimon.) If a superstring is strill orientable during the Regge Action, then the associated superstring becomes tachyonic. This is an example of how a lack of substringular super-symmetry may effect the differential operation of that superstring over a simple Laplacian Transformationm which, if such a condition is integrable over a sequential series of iterations that is non-trivial gauge-metric-wise, will form a Fourier Transformation that involves a superstring that is tachyonic and thereby perturbative relative to its general condition of Noether Flow. Such a perturbation effects the matrix of the delineatory index of the involved orbifolds that are directly effected by this tachyonic multiplicitly integrable distribution. Since the anharmonic multiplicit redistribution of a kinematically unorientable superstring flows differently then the surrounding Noether Conditions, and Noether Conditions are the kinematic delineatory means of maintaining the norm conditions that allow for a sustained covariant Gaussian Symmetry, the Fourier Transformaion involved with a tachyonic flow will produce change in Gaussian Symmetry either via a regular Gaussian Transformation or via a gauge-transformation, the latter of which is the substringular cause of entropy.                


Sincerely, Samuel David Roach. samsphysicsworld@blogspot.com.                                                        

Addendum to course #22

Each iteration that a superstring goes into the Klein bottle, the associated superstring is shuck by a Kaeler metric during Polyakov Action and Bette action before it goes into Regge slope. The associated superstring goes though a minimum of 96 such Kaeler metrics to obtain the metric-gauge that it needs to reattain the permittivity that the said superstring needs to be the energy that it is to be Each shake adds an equal amount of metric-gauge to the given superstring, allowing the superstring mentioned to go into Regge slope each iteration until the associated superstring has 1900% extra potential metric-gauge so that it will not run out of permitivity for a while. The extra potential metric-gauge is stored by 190 smooth and/or Chern-Simmons mini-loops in such a superstring allowing for the superstring to be Yau-Exact or partially Yau-Exact or Chern Simmons while then having the potential for pure hermitian, partially hermitian, or completely non-hermitian singularities in its mini-loops as a vibrating strand or a vibrating hoop. After the 191 iterations of such Kaeler-metric, the said superstring will always be initially orientable and never completely round or straight. The smoothness of the said 191 mini-loops are smooth in 32 spacial derivatives in a 32-dimensional subspace at the locus of the said superstring. The said condition of smoothness is defined by the constancy of each of the 32 derivatives of the said superstring. Such smoothness is Laplacian and thus non-time-oriented. When including the time factor, he Fourier translation of such is smooth or hermitian only per instanton-based observation right before Polyakov and Bette Action. Such hermcity is taken upon a holomorphic polarization detection for forward time moving particles, and such hermicity is taken upon an antihlolomorphic polarization detection for backward time moving particles. Until such a superstring becomes swivel-shaped and/or tachyonic, the 191 mini-loops of such per superstring will remain in number, yet will vary in relative concavity, amplitude, and indistinguishably relative position relative to the surrounding superstrings of the same universe.l As this happens, the norm conditions of the correlative Planck phenomena will maintain their given angling and wobble per iteration relative to the other Planck phenomena, depending on what universe the other Planck phenomena are in, until there is a Gaussian Transformation. The group multiplicit metric of when the Klein bottle raises phenomena equals the duration of the "backgammoning" of the orbifold or orbifold eigenset.